# Competition between exchange-driven dimerization and magnetism in diamond(111)

## TL;DR

This study investigates the competition between structural dimerization and magnetism in the flat surface states of diamond(111), revealing how electron interactions influence insulating and magnetic phases.

## Contribution

It demonstrates that structural dimerization causes insulating behavior, but including spin polarization stabilizes a magnetic, undimerized ground state, highlighting the interplay of structure, electronic, and magnetic properties.

## Key findings

- Dimerization opens an insulating gap in the absence of magnetism.
- Including spin polarization stabilizes a magnetic, undimerized ground state.
- Calculated band gaps are consistent with experimental optical gaps.

## Abstract

Strong electron-electron interaction in ultraflat edge states can be responsible for correlated phases of matter, such as magnetism, charge density wave or superconductivity. Here we consider the diamond(111) surface that, after Pandey reconstruction, presents zig-zag carbon chains, generating a flat surface band. By performing full structural optimization with hybrid functionals and neglecting spin polarization, we find that a substantial dimerization ($0.090$ {\AA} / $0.076$ {\AA} bond disproportionation in the PBE0/HSE06) occurs on the chains; a structural effect absent in calculations based on the LDA/GGA functionals. This dimerization is the primary mechanism for the opening of an insulating gap in the absence of spin polarization. The single-particle direct gap is $1.7$ eV ($1.0$ eV) in the PBE0 (HSE06), comparable with the experimental optical gap of $1.47$ eV, and on the larger(smaller) side of the estimated experimental single particle gap window of 1.57-1.87 eV, after inclusion of excitonic effects. However, by including spin polarization in the calculation, we find that the exchange interaction stabilizes a different ground state, undimerized, with no net magnetization and ferrimagnetic along the Pandey $\pi$-chains with magnetic moments as large as $0.2-0.3~\mu_B$ in the PBE0. The direct single-particle band gap in the equal spin-channel is approximately $2.2$ eV ($1.5$ eV) with the PBE0 (HSE06) functional. Our work is relevant for systems with flat bands in general and wherever the interplay between structural, electronic and magnetic degrees of freedom is crucial, as in twisted bilayer graphene, IVB atoms on IVB(111) surfaces such as Pb/Si(111) or molecular crystals.